Pulsed detonation engines for reaction control systems

ABSTRACT

Pulsed detonation engines (PDEs) are adapted for use in reaction control systems (RCS), such as thrusters for orbital correction and control (e.g., for earth-orbiting satellites), divert thrust generation and control for space-based interceptor devices, and for missile trajectory correction and motion control. According to one aspect of the invention, PDEs are adapted for motion control of so-called “kill vehicles,” which are small devices, typically launched from satellites, for strategic missile defense.

CROSS REFERENCE TO RELATED APPLICATION

This application is a continuation of application Ser. No. 10/796,279,filed Mar. 10, 2004, which claims benefit under 35 U.S.C. § 119(e) toApplication No. 60/320,001, filed Mar. 11, 2003, the disclosures ofwhich are hereby incorporated by reference in their entireties.

FIELD OF THE INVENTION

The present invention is directed to pulsed detonation engines, and moreparticularly to pulsed detonation engines adapted for use in reactioncontrol systems.

DESCRIPTION OF RELATED ART

Reaction control systems (RCS) are conventionally used to correct theorbit or otherwise maneuver a spacecraft or rocket. Examples of reactioncontrol systems include attitude control systems (ACS) and divertengines. The ability to deliver very small thrust impulses is veryimportant for accurate and efficient control of rocket or spacecraftmotion.

In conventional rocket engines, reactive materials are injected into acombustion chamber in which the materials react at high pressure andhigh temperature in a continuous flow process. After reaction in thecombustion chamber, the reaction products expand through a convergingdiverging nozzle, reaching high velocities thereby generating thrust. Ingeneral, the efficiency of the conventional rocket engine is a functionof the temperature in the combustion chamber. Because temperatures inthe combustion chamber often are higher than 2000° C., the structuralelements (e.g., combustion chamber, nozzles, etc.) generally are madefrom materials having very high thermal stability, such as refractorymetal alloys and metal/ceramic composites. Such highly thermally stablematerials are expensive, leading to high costs for the rocket systems.In addition, the need to raise the temperature in the combustion chamberbefore engine operation leads to an increase in minimum thrust pulseduration and engine response time. In small conventional rocket engines,the minimum thrust pulse duration usually is more than 20 msec. Togetherthese factors negatively affect the controlling capability of theengine, limiting its effectiveness in reaction control systems.

In a pulsed detonation engine (PDE), the intermittent mode of operationenables thrust to be produced without the need for pre-heating theengine volume. Thrust is produced when reactive materials injected intothe detonation chamber are ignited and detonated, producing highpressure/high temperature detonation products in the detonation chamber.Because the detonation phase of the PDE cycle is followed by injectionof relatively low-temperature reactive materials, the detonation chamberis cooled by the injection of the fresh reactive materials. It would bedesirable to develop PDEs adapted for providing efficient, highperformance and cost-effective thrust generation in reaction controlsystems.

SUMMARY OF THE INVENTION

The pulsed detonation engines (PDEs) of the present invention areadapted for use in reaction control systems (RCS), such as thrusters fororbital correction and control (e.g., for earth-orbiting satellites),divert thrust generation and control for space-based interceptordevices, and for missile trajectory correction and motion control.According to one aspect of the invention, PDEs are adapted for motioncontrol of so-called “kill vehicles,” which are small devices, typicallylaunched from satellites, for missile interception and neutralization(sometimes referred to as strategic missile defense or “Star Wars”). ThePDEs of the present invention employ one or more of the features asdescribed herein to provide high performance and effective reactioncontrol systems.

According to one aspect, a reaction control system for controllingmotion of a spacecraft or other vehicle is provided. The reactioncontrol system comprises at least one pulsed detonation enginecomprising one or more propellant valves, an igniter, a detonationchamber, and a nozzle. The pulsed detonation engine(s) is/are adapted tocontrollably ignite detonation of a propellant to generate thrust in apredetermined vector for controlling motion of the spacecraft or othervehicle.

According to another aspect, a method of controlling motion of aspacecraft or other vehicle with a reaction control system is provided.The method comprises generating thrust in a predetermined vector bycontrollably igniting detonation of a propellant in at least one pulseddetonation engine in the reaction control system.

BRIEF DESCRIPTION OF THE DRAWINGS

The present invention will now be described in more detail withreference to preferred embodiments of the invention, given only by wayof example, and illustrated in the accompanying drawings in which:

FIG. 1 is a schematic illustration of a pulsed detonation engine for areaction control system in accordance with one embodiment of the presentinvention;

FIG. 2 is a cross-sectional view of a pulsed detonation engine assemblyhaving a plurality of channels within a solid cylindrical body inaccordance with one embodiment of the present invention;

FIG. 3 is a perspective view of a pulsed detonation engine assemblyhaving a plurality of channels within a solid body having a rectangularcross-section in accordance with an alternative embodiment of theinvention;

FIG. 4 is a schematic illustration of a pulsed detonation engine havinga converging/diverging nozzle for injecting a propellant into thedetonation chamber in accordance with an alternative embodiment of theinvention;

FIG. 5 is a schematic illustration of four PDEs assembled into cruciformforming a reaction control system (RCS) for generating thrust to inducespacecraft or missile motion in a required direction for spacecraft ormissile motion control;

FIGS. 6A-6B are graphical illustrations of typical detonation waveformand thrust as a function of time;

FIGS. 7A-7B are graphical illustrations of pressure time history for 400Hz operation with the distance between transducers at 2.5 cm anddetonation wave velocity of about 2 km/sec;

FIG. 8 is a graphical illustration of thrust measured using a pendulumtest cell; and

FIG. 9 is a graphical illustration of thrust as a function of engineoperation frequency.

DETAILED DESCRIPTION OF THE INVENTION

The pulsed detonation engine (PDE) of the present invention operates byintermittent injection and detonation, thereby producing thrust withoutrequiring that the engine volume be pre-heated prior to operation, as isrequired for operation of conventional rocket engines. The intermittentinjection of the relatively low-temperature reactants cools the enginevolume between detonations, leading to only a gradual temperature riseduring engine operation. Because only short intervals of operation areneeded for many reaction control system applications, excessivetemperatures can be avoided. For many applications, this may eliminatethe need for the use of expensive materials in engine construction, suchas refractory metal alloys and metal/ceramic composites as typically areused in conventional rocket engines.

The interval of operation (i.e., the amount of time that theintermittent injection and detonation process occurs withoutinterruption) for the PDE of the present invention can be suitablyselected to facilitate motion control needed for a particularapplication. Depending on such factors as the extent of motioncorrection needed and the mass of the vehicle, for example, the intervalof operation may be very short (e.g., one second or less) orsignificantly longer, for example in the case of auxiliary thrustgeneration. There is no particular minimum interval of operationcontemplated; a very short interval of operation at a high frequency,for example, may be useful to generate a sufficient amount of thrustneeded for a particular application. The interval of operation can be aslong as necessary to provide the requisite thrust, but of course shouldnot result in engine overheating or failure.

The operation of PDEs in RCS is a function of orbit or trajectorycorrection that is required by the control system. For some orbitcorrection maneuvers, the PDEs may be required to generate singleimpulses of thrust every hour or once per day, for example, where otherapplications may require the PDE to operate at a given frequency withoutinterruption for 60 seconds, for example, to facilitate a rapid changein trajectory.

The operational frequency of the PDE can vary over a wide range. By wayof example, the frequency may range from about 0.001 to 1,000 Hz, andoften ranges from about 1 to 500 Hz. The minimum frequencies referencedabove are merely illustrative. It is possible, for example, that a givenorbit correction may be accomplished with a single pulse produced onceper year. Because higher frequencies translate to shorter coolingperiods between detonations, higher frequencies tend to result in fasterrates of engine temperature increase, which may in turn limit themaximum interval of operation. At lower frequencies, adequate coolingmay occur between detonations so as to permit indefinite intervals ofoperation (e.g., not limited by temperature increases). Optionally, thefrequency can be varied during a given interval of operation. Forexample, the PDE may operate initially at a lower frequency which isgradually increased during the interval of operation. This can permitaccurate and rapid correction of spacecraft motion, for example, whileavoiding over-correction or unwanted oscillation of the spacecraft.

Particularly when operating at higher frequencies, it is possible thatdetonation products produced during a given detonation cycle will stillbe present in the detonation chamber at the time propellant is injectedfor the next detonation cycle. The high-temperature detonation productspotentially can ignite the injected propellant prematurely. This canlead to a continuous reaction (effectively combustion) which generallyis undesirable. To avoid unintended self-ignition of the propellant,water or other inert fluid can be injected into detonation chamber toflush the chamber before each cycle or as otherwise may be needed.

According to another aspect of the invention, the PDE employsintermittent injection and detonation with controlled injection times.The controlled injection times usually range from 0.01 to 1,000 msec,more often from about 0.1 to 10 msec. Short injection times permit thedetonable mixture to rapidly fill the detonation chamber, which makesoperation at higher frequencies possible. The controlled injection timecan be suitably selected in accordance with such parameters as theoperational frequency, propellant type and phase, and propellant loadingdensity, to meet the needs of a particular application. It should beunderstood that the controlled injection times indicated above aremerely exemplary and not limiting. It is contemplated that in someapplications, for instance, a significantly longer injection time may beemployed. For example, if only infrequent operation of the PDE isneeded, a propellant may be provided by slowly decomposing water toprovide a hydrogen/oxygen propellant.

It may be advantageous to briefly delay ignition following injection ofthe detonable mixture. The delay can permit better dispersion of thedetonable mixture in the detonation chamber and mixing of propellantcomponents when bi-propellant mixture is used. Also, ignition can bedelayed to allow better condition of mixture initiation in the vicinityof the igniter. Following the completion of injection, ignition can bedelayed from 0 to about 100 msec, more usually from about 0.1 to about10 msec. Preferably, excessive delay periods are avoided because some orall of the injected detonable mixture may escape from the detonationchamber. In addition, longer delay periods will limit the range ofoperation frequencies, which are intrinsically limited by the total timeof injection and ignition.

FIG. 1 illustrates the components of a pulsed detonation engine 1 inaccordance with one embodiment of the present invention. The engine 1includes a detonation chamber 10 and a nozzle 11. The nozzle 11 may be adiverging nozzle, as illustrated in FIG. 1, or may have any othersuitable geometric configuration, such as cylindrical, conical,converging-diverging, and the like. A set of electronically controlledpropellant valves 3 a, 3 b and an integrated injection/ mixing head 2are provided for controlling flow of propellant injected into thedetonation chamber 10. The injected propellant forms a detonable mixturethat fills the detonation chamber 10. A suitable igniter 4, such as aspark plug, laser, pyrotechnic device, etc., is provided in thedetonation chamber 10 to ignite the detonable propellant mixture,producing detonation products. As shown in FIG. 1, the igniter 4 can belocated proximate to the propellant valves 3 a, 3 b. Alternatively, theigniter 4 can be somewhat spaced from the propellant injection point,e.g., by from about 0.1 to 10 cm, at some point along the detonationchamber 10 wall. Varying the position of the igniter 4 permits somecontrol over propagation of the detonation wave and may help maintaincontainment of the detonation products.

The detonation reaction produces a brief period of extremely hightemperature and high pressure inside the detonation chamber 10. Typicaldetonation temperatures are on the order of 4000 K and pressures on theorder of 20-40 atmospheres. Detonation pressure is a direct function ofpropellant density in the detonation chamber and can reach 20,000atmospheres, for example, if the initial average density is about 1g/cc.

The dimensions of the PDE as well as its individual components may varyover a wide range depending on the requirements of a particularapplication, and the present invention should not be construed as beinglimited to any particular dimensions or geometrical configurations. Byway of example, the length of the PDE may range from about 5 to about100 mm, more preferably from about 5 to about 55 mm. The diameter of thedetonation chamber 10 may range from about 0.01 mm to 10 mm. Thesedimensions should be regarded as exemplary and not limiting. It iscontemplated that devices having significantly smaller or significantlylarger dimensions can be made and used in accordance with the principlesof the present invention. In addition, the detonation chamber may benon-cylindrical, i.e., may have a non-circular and/or variablecross-section. Because temperatures of the engine can be kept moderate,as described herein, the geometry of the engine is not limited tocylindrical configurations that traditionally have been required toavoid overheating and dimensional failure. The geometry of the engineinstead can be selected to most effectively adapt to the geometry of thecontrolled vehicle, to most effectively generate the required thrustvectors, or for other considerations.

In one embodiment, a solid body houses a plurality of pulsed detonationengines formed as channels through the solid body. The geometry of thesolid body can be of any suitable configuration. Solid bodies in theform of a cylinder or ring may be advantageous by providing thecapability of generating thrust in a wide variety of directions, whichprovides a high degree of vector control. In some cases, full detonationvelocities can be achieved in channels of only about 0.5 cm in length.The body can be constructed of any suitable material, includinglightweight materials, such as light metals, composites, ceramics, orplastics. Depending on the dielectric properties of the material used, adielectric or electrode pin(s) may be installed along the walls of thedetonation chambers.

As shown in FIG. 2, a PDE assembly 200 can have a plurality of channels205 a-205 g drilled or molded into a solid body 210 at a variety ofradial angles. The channels 205 a-205 g form the detonation chambers ofthe individual PDEs. The channels 205 a-205 g can be of any suitabledimensions, and even can be of micron size, e.g., as small as about 10to 100 μm in diameter. Narrower channels generally provide for bettercooling and improved containment of the detonation products. Thepropellant can be supplied to the center of the body 210 and injectedinto the channels 205 a-205 g. A plurality of igniters 220 a-220 g areprovided in the channels 205 a-205 g proximate to the center of the ringor, alternatively, positioned at intermediate points along the walls ofthe channels 205 a-205 g. The ignition system can be integrated into thesolid body 210.

A common (e.g., single) valve may control injection of the propellantinto the plurality of channels. This enables each channel to have areduced radius. The reduced-radius channels permit the detonation waveto propagate through the propellant to reach effective detonationvelocities and pressures while maintaining containment of the detonationproducts. As schematically shown in FIG. 2, a rotatable valve 225 may beprovided in the center portion of the solid body 210 to selectivelyinject propellant into the individual channels 205 a-205 g.Alternatively, a valve may be configured to simultaneously injectpropellant into two or more channels 205 a-205 g. The small size of thechannels 205 a-205 g permits the injection orifices of the individualchannels to be selectively opened and closed using adaptive structuretechnology, such as piezoelectric, thermo-fluidic, electromagnetic, orsolid state microelectronic mechanical (MEM) systems. The small size ofthe overall device enables other operations such as injection, ignition,and nozzle actuation to be implemented using a controller, such as theaforementioned piezoelectric, thermo-fluidic, electromagnetic, ormicroelectronic mechanical (MEM) systems.

FIG. 3 shows another embodiment of the invention in which a pulseddetonation engine assembly 300 is a solid elongate body 310 having arectangular cross-section. The solid body 310 has a plurality ofchannels 305 a-305 f drilled or molded therein. The remaining details ofthe assembly 300 can be essentially as described above with respect tothe embodiment of FIG. 2.

A wide variety of propellants can be used with the PDE of the presentinvention. Non-limiting examples include fuels detonable in mixtureswith oxygen or other oxidizers such as hydrogen, methane, propane,acetylene, or propylene. Also, detonable mixtures of liquid fuels andoxidizer can be used, e.g., kerosene/oxidizer, alcohol/oxidizer,benzene/oxidizer and other similar mixtures. Detonable mono-propellantsalso can be used, such as nitromethane, nitroglycerin, or similarsingle-component propellants. Bi- and tri-propellant mixtures also canbe used. In space applications, it may be advantageous to use detonablemonopropellant such as nitromethane, nitroglycerin, hydrazine, orbipropellant such as H₂O₂/nitromethane or H₂O₂/kerosene. Other usefulpropellants include aluminum (solid or vapor), magnesium (solid orvapor), carbon, and boron. In general, the propellant can be solid,liquid, vapor, or multi-phase (e.g., dispersion of liquid particles).

In one embodiment, a mixture of tetranitromethane and nitrobenzene isused as propellant. The two components can be mixed over a range ofratios, but preferably the ratio is at or near stoichiometric, e.g.,about 70/30 (tetranitromethane/nitrobenzene). In another embodiment, amixture of tetranitromethane and toluene is employed as propellant.Mixtures of tetranitromethane and toluene are useful over a range ofratios, including, for example, a mixture of about 90/10tetranitromethane/toluene.

The propellant and ignition system preferably are selected to permitsmall size implementation as well as operation of the PDE in vacuum orlow pressure (e.g., as is encountered at high altitudes). Preferredpropellants can be initiated by electric discharge in which the energyof discharge is less than about 5 J, and even as low as about 5 mJ orless.

An energy regeneration and storage device may be provided to permitremote operation of the PDE for extended periods of time. A regenerativeignition system may be employed in which high voltage electrical energyis produced by piezoelectric materials being activated by shock wavesthat are produced during detonation.

For vacuum operation, a restrictive and/or converging nozzle (not shown)may be provided to prevent the detonable mixture from escaping from thedetonation chamber. When using liquid or multi-phase propellants havinga low vapor pressure, the propellant may remain in liquid or liquidparticle form, which may be more easy to contain in the detonationchamber due to lower average loading density of the propellant into thedetonation chamber.

In accordance with one embodiment of the present invention, liquidpropellants are used with a propellant loading density of from about0.001 g/cc to about 0.5 g/cc. Propellant loading densities in this rangeshould be particularly advantageous for RCS applications. One advantageis that excessively high pressures (e.g., on the order of 1 GPa typicalof detonation) can be avoided. Such high pressures are undesirablebecause they can result in loss of containment of the detonationproducts as well as engine damage. Lowering propellant loading densitiesto values less than 0.5 g/cc can result in detonation products pressuresnot exceeding about 0.25 GPa. Such pressures both facilitate containmentof detonation products and help avoid engine rupture.

A propellant-rich gas based on aluminum can be generated without theundesirable formation of an oxide layer. The aluminum particle sizeshould be kept below 10 microns to maintain a sustained detonation.Aluminum also can be generated as a vapor, which will further enhanceits detonability in the presence of a liquid or gaseous oxidizer.Magnesium can be generated as a solid or vapor suspension, and can bedetonated with an oxidizer. The magnesium particles or droplets shouldbe approximately 10 microns or less to detonate. Both aluminum andmagnesium vapor suspensions have very favorable detonation properties.However, an undesirable property of the vapor suspensions is theirtendency to condense on cold surfaces because of the relatively highmelting points of the two metals. Condensation of aluminum and magnesiumvapor can cause mechanical problems if it occurs on tightly fittingparts with small gap tolerances. Alternatively, the system can be heatedby designing a gas generator propellant grain that first produces hotgas followed by the propellant-rich gases.

Nanoscale materials, such as aluminum or boron powder, can be mixed witha propellant to manipulate the properties of the propellant. In oneaspect, nanoscale materials are added to a liquid propellant to activatethe propellant. Nanoscale materials also may be used to reducedetonation velocity and pressure, which helps promote containment. Inaddition, nanoscale materials can be used to increase or decrease thedielectric properties of the propellant (to permit sparking to occur).Persons skilled in the art can determine the relative amount ofnanoscale materials needed to alter the properties of the propellant asdesired with the aid of no more than routine experimentation. Thepropellant activation effect generally occurs when using concentrationsof nanoscale particles on the order of about 0.1 to 1 wt %, whereasreduction of the detonation velocity generally occurs when usingnanoscale particle concentrations of about 1 to 15 wt %. Alternatively,the properties of the propellant can be modified using chemicaladditives.

Particles such as carbon structures, e.g., fullerines, nanotubes, andnanoscale diamond, can be used as propellant additives or as fuel. Also,in some cases nanoscale particles can absorb fuel on their surface,rendering the nanoscale particles detonable.

To ensure the optimum condition for propellant detonation, the fuel andoxidizer should be thoroughly mixed to ensure the fuel concentration iswithin the detonability limit (i.e., near stoichiometric). Mixing can becharacterized on several levels including macroscopic and microscopicscales. Macroscopic mixing refers to the bulk fluid processes, whichbring the fuel and oxidizer components to close proximity (e.g.,impingement of fuel and oxidizer streams). Microscopic mixing is theprocess by which the fuel and oxidizer are further mixed to a lengthscale required for detonation. Many techniques can be employed toproduce microscopic mixing.

The propellant can be injected into the detonation chamber, and ignitedwhen it is in the dispersed phase. Detonation thus can be initiated whenthe dispersed propellant is not confined by the walls of the detonationchamber. This reduces the loading density (e.g., to about 1 g/cc) andpressure inside of the detonation chamber, which assist withcontainment. A groove (not illustrated) or other structure may beprovided within the detonation chamber to contain or partially containthe injected propellant. The propellant may be partially contained in agroove, for example, so that upon detonation, the detonation productsare allowed to rapidly expand laterally, thus reducing pressure in thechamber. Alternatively, the detonable mixture can be dispersed within athin layer around the inside surface of the detonation chamber walls.The thin layer permits the detonation products to expand while limitingthe detonation pressure reached, e.g., to avoid excessively largepressure or explosion.

As illustrated in FIG. 4, it may be advantageous to inject a gaseous,multi-phase, or liquid propellant (represented by arrow A) into thedetonation chamber 10 with a converging/diverging nozzle 19 when thepropellant is detonated with a pressure in the detonation chamber 10that is larger than the pressure outside of the nozzle 19. The igniter 4can be positioned along the wall of the detonation chamber 10, e.g.,downstream of the point of propellant injection.

Several methods for initiating a detonation cycle may be used.Detonation may be initiated by igniting a fuel-oxygen mixture in a smalldetonation tube (not illustrated) that discharges into the detonationchamber, or by igniting a fuel-oxygen mixture collocated within thedetonation chamber. Alternatively, a high voltage electric discharge orpyrotechnic igniter can be used. The small detonation tube methodgenerally requires fuel, an oxidizer, pumps, high-speed fluid valves, anelectronic controller, a power supply and a spark generator. The directelectric discharge method generally requires a spark plug, an electroniccontroller and a power supply. Laser ignition can be used, where a laserproduces a high-energy beam initiating detonation of propellant in thedetonation chamber.

In one embodiment of the present invention, relatively low detonationvelocities, e.g., from about 1 to 5 km/s, are employed. Conventionaldetonation velocities range from about 6 to 8 km/s. Various techniquesmay be used for controlling detonation velocities. One technique forlimiting detonation velocity is selecting a detonation chamber geometryto limit the detonation wave propagation. Another technique is toprovide additives to liquid propellants that will reduce detonation wavevelocity and pressure. Yet another technique is selecting a propellantthat provides relatively low pressure of detonation products.

The PDE of the present invention can be used alone or in combinationwith one or more additional PDEs for generating thrust. The thrustgenerated during the interval of operation, as previously described, isparticularly useful in various applications reaction control systems,such as orbital control for earth-orbiting satellites. The PDE may bemounted onto a satellite such that its operation produces thrust in aparticular direction or vector. Optionally, the PDE is mounted onto arobotic device, which enables the PDE to be rotated along one or moreaxes to vary the direction of thrust. Two or more PDEs can be actuatedsimultaneously or sequentially.

Simultaneous actuation of multiple PDEs can be used, for example, toincrease the total amount of thrust generated during an interval ofoperation or to generate thrust vector in a particular direction.Sequential actuation of two or more PDEs may be desirable in cases wherea longer period of thrust is needed. For example, a first PDE can beactuated for a first interval and then cooled for a period during whichoperation of a second PDE for a second interval continues thrustgeneration. If even longer periods of thrust are needed, the first andsecond (and possibly additional) PDEs can be operated cyclically forextended periods of thrust generation.

FIG. 5 illustrates four PDEs 1 a, 1 b, 1 c, and 1 d assembled into acruciform, forming a reaction control system (RCS) for generatingthrust, e.g., to induce motion of a spacecraft, missile, or othervehicle in a required vector. Each of the PDEs 1 a, 1 b, 1 c, and 1 dincludes electronically controlled propellant valves 3 a′ and 3 b′, anigniter 4′, and other features as previously described.

FIGS. 6A and 6B illustrate pressure distribution of a detonation wavepropagating through the detonation chamber. The detonation wave travelsat a velocity of about 2 km/sec. Thrust is produced when the pressure onthe thrust wall and nozzle is higher than the ambient pressure and isgenerated continuously until the rarefaction wave arrives from the aftend of the engine and reduces the pressure to negligible levels. Theforce produced by detonation can be calculated by direct integration ofthe pressure over the projections of the internal and external surfacesof the engine onto the plane normal to the direction of motion.

In FIGS. 7A and 7B, it can be observed that low initial pressure in thedetonation chamber allows injection of detonable liquids directly fromthe propellant tank without the need of a compressor as is used inconventional rocket systems to raise the injection pressure to thepressure in the combustion chamber (usually to about 1,000-10,000 psi).In FIGS. 7A and 7B, pressure time histories for pressure transducerslocated at 2.5 cm, 5 cm, and 7.5 cm from the injection points are shown.FIG. 7A shows the pressure record for a 0.1 sec interval when the enginewas operated at 400 Hz (the pressure spikes correspond to detonationevery 2.5 msec). The variation of the peak pressure value in FIG. 7A isa measurement artifact related to construction of the pressuretransducers. FIG. 7B shows a 0.1 msec interval, showing pressure for asingle detonation. FIGS. 7A and 7B illustrate very regular engineoperation at high frequency. Measurement of time between the shock wavesin FIG. 7B shows that a fully developed, 2 km/sec detonation wavepropagates through the mixture. This device generates thrust in 400 bitsper second with about 15 millinewton per bit. The duration of the bitimpulse is about 0.2 msec.

In FIG. 8, thrust as a function of time is shown for 400 Hz frequencyoperation. This record is produced by a calibrated gonionometer thatrecords the thrust produced by the engine attached to the pendulum.

In FIG. 9, thrust as a function of detonation frequency is shown for thetest regime when only half of the engine volume was filled with thepropellant. FIG. 9 shows that thrust is a direct function of frequency.

While particular embodiments of the present invention have beendescribed and illustrated, it should be understood that the invention isnot limited thereto since modifications may be made by persons skilledin the art. The present application contemplates any and allmodifications that fall within the spirit and scope of the underlyinginvention disclosed and claimed herein.

1. A reaction control system for controlling motion of a vehicle, thereaction control system comprising: at least one pulsed detonationengine comprising one or more propellant valves, an igniter, adetonation chamber, and a nozzle; wherein the at least one pulseddetonation engine is adapted to controllably ignite detonation of apropellant to generate thrust in a predetermined vector for controllingmotion of said vehicle.
 2. The reaction control system of claim 1 whichcomprises a plurality of pulsed detonation engines capable of generatingthrust in a plurality of vectors.
 3. The reaction control system ofclaim 2 further comprising a controller for controlling operation ofsaid plurality of pulsed detonation engines, wherein the controller isselected from the group consisting of a piezoelectric device, athermo-fluidic device, a microelectronic mechanical system, anelectromagnetic system, and combinations thereof.
 4. The reactioncontrol system of claim 1 wherein said at least one pulsed detonationengine comprises a detonation chamber having an igniter positioneddownstream of a point at which propellant is injected.
 5. The reactioncontrol system of claim 1 wherein said at least one pulsed detonationengine comprises an igniter selected from the group consisting of aspark plug, a pyrotechnic device, and a laser.
 6. The reaction controlsystem of claim 1 further comprising an electrical energy regenerationand storage device capable of permitting remote operation of said atleast one pulsed detonation engine for extended periods of time.
 7. Avehicle comprising the reaction control system of claim
 1. 8. A reactioncontrol system for controlling the motion of a missile or other vehicle,the reaction control system comprising: at least four pulsed detonationengines arranged in a cruciform for selectively generating thrust in atleast four vectors, wherein each of said pulsed detonation enginescomprises electronically controlled propellant valves, an igniter, adetonation chamber, and a nozzle; a controller for selectively actuatingsaid at least four pulsed detonation engines, the controller comprisingat least one of a piezoelectric device, a thermo-fluidic device, anelectromagnetic device, and a microelectronic mechanical system.
 9. Amissile comprising the reaction control system of claim
 8. 10-34.(canceled)
 35. The reaction control system of claim 1 which is athruster for orbital correction and control of an earth-orbitingsatellite.
 36. The reaction control system of claim 1 which providesdivert thrust generation and control for a space-based interceptordevice.
 37. The reaction control system of claim 1 which providestrajectory correction and motion control of a missile.